 |
Section by Section Description
FORCE_FIELD_SETTINGS
Key block (required)
This key block specifies various global options for the force field file,
mostly concerned with the treatment of the non-bonded potentials.
| FORCE_FIELD_SETTINGS |
| ================================ |
| ELSTAT_1-4_SCALE
| 0.5 |
| VDW_1-4_SCALE |
0.5 |
|
| VDW_DEFAULT_POTENTIAL |
1 |
(1:6-12 2:exp-6 3:exp purely repulsive) |
| DIELECTRIC_CONSTANT |
1.000 |
| ================================ |
ELSTAT_1-4_SCALE & VDW_1-4_SCALE
Most force fields scale the non-bonded interactions by a factor of
0.5 if the atoms are the terminal atoms of a defined torsion. This scaling factor, which is termed the 1-4
scaling factor, can also be different for the electrostatic potential and for
the Van der Waals potentials and thus they are separately defined in the input.
VDW_DEFAULT_POTENTIAL
This keyword defines what kind of potential is used for the
non-bonded van der Waals interactions. The potential types have been assigned
integer values as defined in the following table.
| VDW potential type |
|
constants required (in order) |
| 0 |
no potential |
none |
| 1 |
Lennard-Jones 12-6
|
Do, Ro |
| 2 |
Exponential-6 or Buckingham
|
Do, Ro, x x=12.0 is standard |
| 3 |
Purely Repulsive
|
Do, Ro, x |
| 4 |
Purely Attractive (dispersion term)
|
Do, Ro |
DIELECTRIC_CONSTANT
Default = 1.00
This defines the dielectric constant used for the calculation of the
electrostatic interactions. For example, 1.00 = vacuum and 80 is that of bulk
liquid water. Currently, only a
constant dielectric has been implemented.
BONDS
Key block (required)
This key block specifies the potential type and parameters for each kind of MM
bond stretching interaction. An example
is given below.
| BONDS |
| Atoms |
pot |
K |
ro |
NOTES |
| i - j |
type |
(kcal/molA^2) |
(Ang) |
| ========================================= |
| CA |
CA |
1 |
938.0 |
1.400 |
amber95 |
| CT |
CT |
1 |
620.0 |
1.526 |
amber95 |
| HC |
Zr |
0 |
0.0 |
|
no potential found |
| ========================================= |
The first two columns are the atom types (up to four characters long) and the
third column is an integer specifying the potential type.
| BOND potential type |
|
constants required (in order) |
| 0 |
no potential |
none |
| 1 |
simple harmonic:
AMBER95, Sybyl
|
K, Ro |
BENDS
Key block (required)
This key block specifies the potential type and parameters for each kind of MM
bond angle interaction. An example is
given below.
| BENDS |
| Atoms |
pot |
k |
ao |
NOTES |
| i - j - k |
type |
(kcal/mol) |
deg |
| =========================================== |
|
| * |
CA |
* |
1 |
70.00 |
120.00 |
example of wild card |
| * |
CA |
CA |
1 |
126.00 |
120.00 |
| CA |
CA |
N2 |
1 |
140.00 |
120.10 |
amber95 N2-CA-CM |
| CA |
CA |
CT |
1 |
140.00 |
120.00 |
amber95 |
| =========================================== |
|
The first three columns specify the atom types and the fourth column is an
integer specifying the potential type.
The angle bend potential types are described in the table below with the
additional constants required.
| BEND potential type |
|
constants required (in order) |
| 0 |
no potential |
none |
| 1 |
theta harmonic:
AMBER95, SYBYL
|
K,qo (q in degrees) |
Notice that wild cards can be specified for both terminal
positions of the bend or just one as in the example above. It is important that the parameters be
ordered from the least specific (those containing the most wild cards) to the
most specific parameters.
TORSIONS
Key block (required)
This key block specifies the potential type and parameters for each kind of MM
bond torsion interaction. For the bond stretching and bending potentials, only
one potential has to date been implemented since both AMBER and SYBYL both use
simple harmonic potentials. However, AMBER and SYBYL use different functional
forms to represent the torsion potentials, each with their own set of
parameters. The AMBER and SYBYL torsional potentials used in this program are
defined in the table below.
| TORSION potential type |
|
constants required (in order) |
| 0 |
no potential |
none |
| 1 |
AMBER:
|
Ki, ni (periodicity-integer), fo,i
(phase shift) |
| 2 |
SYBYL:
|
K, s |
Notice that the two potentials have a different number of
parameters. For example, when the program reads 'potential type' number 1, it
will expect three parameters Ki, ni, fo,i. Further notice that the
AMBER torsional potential is a sum of Fourier components (this is what the
index i refers to).
Below is an example of the TORSIONS key block, made up of AMBER force field
types.
| TORSIONS |
| Atoms |
pot |
|
per. |
shift |
| i - j - k - l |
type |
k |
n |
to |
NOTES |
| ====================================================== |
| * |
CV |
NB |
* |
1 |
2.4000 |
2 |
180.0 |
JCC,7,(1986),230 |
| * |
CW |
NA |
* |
1 |
1.5000 |
2 |
180.0 |
JCC,7,(1986),230 |
| & |
|
|
|
|
0.1000 |
3 |
0.0 |
| C |
N |
CT |
C |
1 |
0.2000 |
2 |
180.0 |
| N |
CT |
C |
N |
1 |
0.4000 |
4 |
180.0 |
| & |
|
|
|
|
1.3500 |
2 |
180.0 |
| & |
|
|
|
|
0.7500 |
1 |
180.0 |
| CT |
CT |
N |
C |
1 |
0.5000 |
4 |
180.0 |
| ====================================================== |
Most AMBER torsion potentials are not specific to all four atoms i-j-k-l, but
only on the central two, j-k. Wild cards are specified with the '*' symbol as
illustrated above. Again, the ordering is important. The parameters should be
ordered from least specific (those containing the most wild cards) to most
specific. The AMBER torsion potential can be composed of more than one Fourier
component for a single torsion potential.
Additional Fourier components are specified with the '&'
continuation symbol as in the example above. At the moment, up to 6 Fourier
components are allowed. Notice that the individual components need not be
specified in any particular order. In
the above example key block, there are only 5 torsional potentials defined, not
8. Two of the potentials are composed of more than one Fourier component as
indicated by the '&' continuation line.
Below is an example of the TORSIONS key block for the SYBYL force field. Notice
that the potential types are all '2'. There are fewer parameters and no multi
component potentials. Also, some potentials are defined with two or only one
wild card.
| TORSIONS |
| ------------------------------------------- |
| Atoms |
pot |
| i - j - k - l |
type |
k |
per |
NOTES |
| =============================================== |
| * |
C_ar |
S_3 |
* |
2 |
1.0000 |
3.0 |
* |
| * |
S_3 |
S_3 |
* |
2 |
0.0000 |
2.0 |
EXP |
| C_2 |
C_2 |
C_3 |
* |
2 |
0.1260 |
-3.0 |
WHITE_77 |
| C_3 |
C_2 |
C_3 |
* |
2 |
0.1260 |
3.0 |
WHITE_77 |
| H |
C_2 |
C_3 |
* |
2 |
0.2740 |
3.0 |
* |
| * |
C_ar |
C_ar |
C_ar |
2 |
2.3500 |
-2.0 |
* |
| * |
C_2 |
C_3 |
C_2 |
2 |
0.1260 |
3.0 |
WHITE_77 |
| * |
C_2 |
C_3 |
C_3 |
2 |
0.1260 |
3.0 |
WHITE_77 |
| * |
C_2 |
C_3 |
H |
2 |
0.2740 |
3.0 |
WHITE_77 |
| * |
C_3 |
C_3 |
H |
2 |
0.3200 |
3.0 |
MC_88 |
| O_2 |
C_2 |
C_3 |
C_3 |
2 |
0.7000 |
-3.0 |
JL_ES_ |
| O_co |
C_2 |
C_3 |
C_3 |
2 |
0.7000 |
-3.0 |
MAC_1 |
| C_2 |
C_3 |
C_3 |
C_2 |
2 |
0.0400 |
3.0 |
WHITE_77 |
| C_2 |
C_3 |
C_3 |
C_3 |
2 |
0.1260 |
3.0 |
WHITE_77 |
| =============================================== |
One can also mix different potential types within the same force field file, as
illustrated below. In this example, three are three potentials. The first two
are SYBYL type potentials whereas the last one is a multi component AMBER
potential.
| H |
C_2 |
C_3 |
* |
2 |
0.2740 |
3.0 |
|
| * |
C_ar |
C_ar |
C_ar |
2 |
2.3500 |
-2.0 |
|
| N |
CT |
C |
N |
1 |
0.4000 |
4 |
180.0 |
| & |
|
|
|
|
1.3500 |
2 |
180.0 |
| & |
|
|
|
|
0.7500 |
1 |
180.0 |
OUT-OF_PLANE
Key block (required)
This key block specifies the potential type and parameters for each kind of MM
out of plane bend. This potential is sometimes referred to as the inversion
potential or improper torsions (depending on the force field). The potential types currently supported are
provided in the table below.
| out-of-plane potential type |
description |
constants required (in order) |
| 0 |
no potential |
none |
| 1 |
AMBER:
|
K, n, fo (n=2, fo
= 180° for planar, n=3, fo
= 120° for tetrahedral)
|
| 2 |
SYBYL:
d is the distance of the plane in Ang.
|
K |
An example of the key block for the AMBER type potentials is
given below. It is important to realize that the atom k is the atom k is the central atom. (We have adopted the somewhat odd standard
of AMBER in this respect).
| OUT-OF-PLANE |
| -------------------------- |
| Atoms |
pot |
| i - j - k - l |
type |
K |
to |
NOTES |
| ============================================= |
| * |
* |
CA |
H4 |
1 |
1.10 |
180.0 |
bsd.on C6H6 nmodes |
| * |
* |
CA |
H5 |
1 |
1.10 |
180.0 |
bsd.on C6H6 nmodes |
| * |
O2 |
C |
O2 |
1 |
10.50 |
180.0 |
JCC,7,(1986),230 |
| * |
N2 |
CA |
N2 |
1 |
10.50 |
180.0 |
JCC,7,(1986),230 |
| * |
CT |
N |
CT |
1 |
1.00 |
180.0 |
JCC,7,(1986),230 |
| CK |
CB |
N* |
CT |
1 |
1.00 |
180.0 |
|
| ============================================= |
VAN DER WAALS
Key block (required)
This key block specifies the potential type and parameters for each kind of MM
van der Waals interaction between two atoms.
A sample key block is shown below:
| atom(s) |
type |
emin |
rmin |
alpha |
NOTES |
| ========================================== |
| CA |
|
-.0860 |
3.81600 |
12.00 |
amber95 |
| HA |
|
-.0150 |
2.91800 |
12.00 |
amber95 |
| Ni - HA |
2 |
-.0480 |
2.7 |
12.00 |
NOTE potential type |
| Ni - CA |
D |
-.0480 |
2.7 |
12.00 |
default potential |
| ========================================== |
The van der Waals key block is somewhat different than the previous key blocks,
because generally not every atom pair is defined with its own parameters.
Rather, the parameters are assigned on a per atom basis and then special
combination rules are used to construct the parameters for each atom pair
combination. For this reason, a default potential type is defined in the FORCE_FIELD_SETTINGS
key block.
| VDW potential type |
|
constants required (in order) |
| 0 |
no potential |
none |
| 1 |
Lennard-Jones 12-6
|
Do, Ro |
| 2 |
Exponential-6 or Buckingham
|
Do, Ro, x x=12.0 is standard |
| 3 |
Purely Repulsive
|
Do, Ro, x |
For each type of van der Waals interaction, the program first
scans the key block for pair specific parameters. For pair specific potentials, the default potential type can be
replaced by any of the available potentials. The three sample lines below
specify pair-specific potentials. The two atom types must be separated by a
hyphen with spaces between the hyphen and the atom type. Following the specification of the atom
pair, the potential type is defined. If
D or d is specified here, then this means to use the default potential type.
Following the potential type are the parameters needed for that potential type
(see above table).
| CA - CA |
1 |
0.0860 |
3.81600 |
12.00 |
amber95 |
| Ni - HA |
0 |
| Ni - CA |
D |
0.0480 |
2.7 |
12.00 |
default potential type |
If a pair specific parameter can't be found, then the program looks for
individual atom parameters corresponding to each of the atom types in the
pair. The pair specific parameters are
then constructed from combination of the two individual atom parameters using
the following combination rules:
| VDW potential type |
|
|
| 1 |
Lennard-Jones 12-6 |
Dij = (Di*Dj)1/2,
Rij = (Ri+Rj)/2
|
| 2 |
Exponential-6 or Buckingham |
Dij = (Di*Dj)1/2,
Rij = (Ri+Rj)/2
zij = (zi*zj)1/2
|
| 3 |
Purely Repulsive |
Dij = (Di*Dj)1/2,
Rij = (Ri+Rj)/2
zij = (zi*zj)1/2
|
When individual atom parameters are not used, no potential
type is specified since the default potential type is always used. An example
is given below.
| CA |
0.0860 |
3.81600 |
12.00 |
amber95 |
| HA |
0.0150 |
2.91800 |
12.00 |
amber95 |
The ability to define pair specific parameters is especially useful for those
force fields that have different combination rules than used in the program.
For example, Jorgensen's TIP3P water force field uses geometric averages for
both Dij and Rij.
MASSES & ATOM LABELS
Key block (required)
This key block specifies the default masses for each MM atom type and the
element label for each MM atom type. In an ADF QM/MM run, the element label
defined for each atom type is the label used for printing out to the
LOGFILE. This allows one to easily cut
and paste the generated coordinates to a molecule viewing program without
having to go in and changing all of the "CT"s to "C"s.
A sample key block is shown below:
| MASSES & ATOM LABELS |
| ============================== |
| Ni |
Ni |
58.70 |
| CM |
C |
12.011 |
| CA |
C |
12.011 |
| CT |
C |
12.011 |
| HC |
H |
1.0079 |
| HA |
H |
1.0079 |
| ============================== |
The first column is the MM atom type, the second is the label used for printing
and the third column is the mass of the atom type. The atoms do not have to be specified in any particular order.
CHARGES
Key block (optional)
This key block specifies the parameters for the charges on the atoms by atom
type. To date only the initial charge
is available, however if some sort of charge equilibration scheme was
introduced the parameters would go here.
NOTE: initial charges can also
be specified on a per atom basis in the MM INPUT file.
| CHARGES |
| atoms |
initial |
| label |
charge |
| ======================== |
| OW |
-0.8 |
| HW |
0.4 |
| ======================== |
|